[0001] The present invention relates to a fixed-point cell required to calibrate a thermometer
such as, for example, a radiation thermometer used in a high-temperature region exceeding
1100°C, and to a thermometer calibration method and fixed-point temperature realizing
apparatus using the cell.
[0002] When thermometers are calibrated, at or above a room temperature region, a freezing
point or a melting point of a metal is employed as a defining fixed-point temperature
of the International Temperature Scale of 1990 (ITS-90). A fixed-point cell is used
as a method of realizing the fixed-point temperature. Carbon crucibles, in which pure
metal is cast as a fixed-point material of high melting point, have been usually used
as the fixed-point cell. A thermometer is calibrated utilizing the fact that when
the liquid phase and the solid phase of the fixed-point material coexist in the crucible,
the temperature of the cell is not varied due to the latent heat of the melting. This
is realized by placing the fixed-point cell in a temperature-variable furnace and
observing the temperature variation of the cell when an environmental temperature
is increased and decreased (see Chapter 7 of "New Edition of Proper Use of Thermometer,"
edited by Japan Electric Instrument Manufacturers' Association, published by Nihon
Kogyo Publishing Co. (1997)).
[0003] The maximum fixed-point temperature is the copper point of 1085°C; at temperatures
higher than the copper point the temperature scale is defined by extrapolation. In
the temperature region above the copper point the temperature scale is maintained
by utilizing a radiation thermometer calibrated at a fixed point below the copper
point, or by transferring the radiance temperature to the current of a tungsten ribbon
lamp.
[0004] Attempts to realize a fixed-point temperature in the temperature region above the
copper point include attempts to realize the freezing point of palladium (freezing
point: 1550°C) and platinum (freezing point: 1770°C), and an example where the fixed-point
temperature was measured by melting them using an alumina crucible has been reported
(see T. J. Quinn, T. R. D. Chandler: Temperature, Its Measurement and Control in Science
and Industry, H. H. Plumb, (ed.), Vol. 4, Part 1, p. 295, Pittsburgh: Instrument Society
of America (1972), P. B. Coates, T. R. D. Chandler, J. W. Andrews; High Temperature
and High Pressure, Vol. 15, p. 573 (1983)).
[0005] There has also been reported an attempt at obtaining a fixed-point temperature by
using tungsten as a crucible material, melting alumina therein, observing the melting
and freezing thereof at 2050°C with a radiation thermometer and using that as a fixed-point
temperature (see H. Sakate, F. Sakuma, A. Ono: Metrologia, Vol. 32, p. 129 (1995)).
[0006] On the other hand, an attempt has been made to use metal-metal eutectics as a fixed-point
temperature material. It has been reported that a fixed-point temperature was realized
by casting copper-silver eutectics or copper-aluminum eutectics in a carbon crucible
and observing the melting and freezing thereof (Itoh, Papers Of The Society of Instrumentation
and Control Engineers, Vol. 19, No. 12, p. 978 (1983)).
[0007] One of the present inventors has proposed a fixed-point cell comprising a crucible
composed of carbon, a fixed-point material enclosed in the crucible that is a eutectic
structure of carbon and metal, a fixed-point temperature realizing apparatus using
the fixed-point cell comprising a furnace having the fixed-point cell disposed therein
for increasing and decreasing an environmental temperature of the cell and a thermometer
to measure temperature variations in the cell, and a calibration method for calibrating
the thermometer based on the measured temperature variations (JP-A 2000-180272).
[0008] The maximum temperature of conventional fixed-point cells which use carbon and in
which pure metal is cast is the copper point of 1085°C (Figure 2). This is because
when a metal having a higher melting point is melted in a carbon crucible, the carbon
is dissolved in the metal, reducing the purity of the metal and thereby lowering the
freezing point.
[0009] Thus, there is no fixed-point cell above the copper point, so the temperature scale
is maintained by a ribbon lamp or radiation thermometer. However, the dependency on
extrapolation of the temperature scale thus maintained greatly reduces the accuracy
of the temperature scale. For example, in the case of calibration traceability of
radiation thermometers in Japan, the provided accuracy is 0.3°C at 1085°C, decreasing
sharply to 4°C at 1600°C and to 8°C at 2000°C.
[0010] Moreover, setting a higher-accuracy scale, using a high-accuracy radiation thermometer,
for example, together with the precise evaluation of the thermometer characteristics
and the like, involves a massive effort. However, since it still depends on extrapolation,
the resulting uncertainty in temperature scale realization and maintenance is still
in the region of 0.8°C at 2000°C.
[0011] Also, since the emissivity of the ribbon in a ribbon lamp is not 1, correction is
required depending on the measurement wavelength. In addition to the difficulty of
using a ribbon lamp with high accuracy, the ribbon has to be sealed in an inert gas
atmosphere since the tungsten vaporizes at temperatures above 2000°C. As a result,
stable ribbon lamp characteristics cannot be obtained due to the convection of the
inert gas.
[0012] For realising the palladium point or the platinum point, an alumina crucible can
be used in the measurement for a short period. However, it is not practical for repeated
use because the alumina is brittle and susceptible to thermal shock, making the crucible
thus used prone to breakage, while a further problem is that owing to metal contamination
arising from the alumina reduction, the crucible has to be used in an oxidizing atmosphere.
[0013] The method of melting alumina in a tungsten crucible has low realizability. The reasons
for this include the poor workability of tungsten, the difficulty of sealing molten
alumina into a lateral crucible, and the fact that sufficient accuracy cannot be obtained
since a blackbody cavity whose emissivity is near to 1 cannot be formed due to the
low emissivity of the tungsten.
[0014] The method of using metal-metal eutectics serves the purpose of increasing the number
of fixed-point temperatures in a temperature region lower than the copper point. When
the same method is used in a temperature region higher than the copper point, a fixed-point
temperature cannot be realized because a freezing point is unavoidably lowered by
the dissolution of carbon.
[0015] In the case of the method using a fixed-point cell comprising a crucible composed
of carbon and a fixed-point material in the crucible that is a eutectic structure
of carbon and metal, it is only possible to realize a fixed-point temperature up to
2732°C (Figure 3). As a practical problem, osmium oxide is a colorless, highly-toxic
gas. Considering its unsuitability as a fixed-point substance, as a fixed-point temperature
using a eutectic structure of carbon and metal, the maximum temperature is 2474°C
using a eutectic structure of carbon and rhenium.
[0016] An object of the present invention is to overcome the above shortcomings of the prior
art by providing a fixed-point cell that extends the fixed-point temperature region
to the temperature region exceeding 2500°C and enables the achievement of high calibrating
accuracy in the calibration of all thermometers that are used in a high temperature
region such as radiation thermometers and the like, and a thermometer calibration
method and fixed-point temperature realizing apparatus using the above cell.
[0017] To attain the above object, the present invention provides a fixed-point cell comprising
a crucible composed of carbon and a fixed-point material enclosed in the crucible,
wherein the fixed-point material is a eutectic structure of carbide and carbon.
[0018] A fixed-point temperature realizing apparatus according to the present invention
comprises a fixed-point cell comprising a crucible composed of carbon and a fixed-point
material enclosed in the crusible that is a eutectic structure of carbide and carbon,
and a furnace having the fixed-point cell disposed therein for increasing and decreasing
an environmental temperature of the cell and a thermometer to measure temperature
variation in the cell.
[0019] A calibration method for calibrating a thermometer according to the present invention,
the method comprising enclosing a fixed-point material that is a eutectic structure
of carbide and carbon in a crucible composed of carbon to form a fixed-point cell,
raising and lowering an environmental temperature of the cell, measuring the temperature
variation of the cell with a thermometer to be calibrated, and calibrating the thermometer
based on the measured temperature variation.
[0020] As the carbide, there may be used a carbide of any of boron, molybdenum, vanadium,
titanium, zirconium, hafnium, niobium, tantalum, tungsten, and rare earth elements.
[0021] The thermometer may be a thermometer used for measuring high temperatures such as
a radiation thermometer.
[0022] As described in the foregoing, accurate thermometer calibration can be effected even
in a temperature region exceeding 2500°C by using a fixed-point material having a
eutectic structure of carbide and carbon.
[0023] Further features of the invention, its nature and various advantages will be more
apparent from the detailed description of the invention made with reference to the
accompanying drawings, in which:-
Figure 1 is a sectional view showing an embodiment of a fixed-point cell according
to the present invention,
Figure 2 shows pure-metal fixed-point temperatures in accordance with ITS-90,
Figure 3 shows the fixed-point temperatures of metal-carbon eutectic structures described
in JP-A 2000-180272,
Figure 4(a) shows fixed-point temperatures of eutectic structures of metal carbide
and carbon used in the present invention,
Figure 4(b) shows fixed-point temperatures of eutectic structures of rare earth carbide
and carbon used in the present invention,
Figure 5 is an example of a diagram showing the phase of carbide-carbon eutectic material
used in the present invention,
Figure 6 is a sectional view of an embodiment of the fixed-point temperature realizing
apparatus according to the present invention,
Figure 7 shows an example of the output of a thermometer to be calibrated according
to the embodiment of Figure 6, and
Figure 8 is a sectional view of another embodiment of the fixed-point temperature
realizing apparatus according to the present invention.
[0024] Embodiments of a fixed-point cell, and a fixed-point temperature realizing apparatus
and thermometer calibration method using the cell, will now be described below, with
reference to the accompanying drawings.
[0025] Figure 1 is a sectional view showing an embodiment of a fixed-point cell 4 according
to the present invention, comprising a crucible 1 and a carbide-carbon eutectic structure
2 enclosed in the crucible 1. The temperature of the melting point and the freezing
point of the eutectic structure 2 is used as a fixed-point temperature. Reference
numeral 3 denotes a blackbody cavity.
[0026] The fixed-point cell 4 calibrates a thermometer to be calibrated by disposing the
cell in a temperature-variable electric furnace, measuring the temperature variation
therein with the thermometer when an environmental temperature is increased and decreased
and making use of the fact that when the liquid phase and the solid phase of the fixed-point
material coexist in the cell, the temperature variation disappears due to the latent
heat of the melting. The thermometer to be calibrated can be any of various types
of thermometer used at high temperatures such as a radiation thermometer and a thermocouple
and the like. The carbide materials used in the cell are ones that form carbon eutectics
whose melting point is higher than the copper point. Specifically, there may be used
a carbide of any of boron, molybdenum, vanadium, titanium, zirconium, hafnium, niobium,
tantalum, tungsten, and rare earth elements.
[0027] Figure 2 shows pure-metal fixed-point temperatures in accordance with ITS-90, conventionally
used at above ambient temperatures, in which reference symbol f.p. denotes a freezing
point, m.p. a melting point and t.p. a triple point, and Figure 3 shows the fixed-point
temperatures of metal-carbon eutectic structures described in JP-A 2000-180272. From
Figure 2, it can be seen that in the case of the cell in which pure metal is cast,
the copper point of 1085°C is the maximum temperature. On the other hand, in the case
of a fixed-point cell with a fixed-point material composed of a carbon-metal eutectic,
as shown in Figure 3, the maximum temperature is 2474°C using a practicable rhenium
eutectic structure.
[0028] Figures 4(a) and 4(b) show fixed-point temperatures of carbide-carbon eutectic structures
used in the present invention, and Figure 5 is an example of a diagram showing the
phase of titanium-carbon used in the present invention.
[0029] The operation of the fixed-point cell of the present invention will now be described
with reference to Figures 4 and 5. While the freezing point of titanium carbide (TiC)
is 3067°C, it can be seen from Figure 5 that the fixed-point eutectic used in the
present invention has a freezing point temperature of 2776°C in a composition ratio
containing 30 wt% of carbon.
[0030] If the melting point is exceeded, there is some dissolution of the carbon of the
crucible. However, when the temperature is again decreased, the composition ratio
of the eutectic is recovered when the freezing point is reached because excess carbon
is precipitated. As a result, melting and freezing plateaus having good reproducibility
can be observed. Also, since the carbide-carbon eutectic uses the same material as
the crucible, the crucible material is intrinsically free of impurities from the crucible,
so the freezing point does not drop. Moreover, since carbon is used for the crucible,
there is no problem with respect to crucible durability, in contrast to when an alumina
crucible is used. Furthermore, when the eutectic to which carbon was added beforehand
is melted at the eutectic composition ratio thereof, there is only slight dissolution
of the carbon from the crucible, and the crucible durability is not degraded by the
melting.
[0031] In addition, since carbon having high emissivity is used as the crucible material,
a blackbody cavity 3 having sufficiently high emissivity can be readily formed and
is also suitable for calibrating a radiation thermometer. A thermometer calibrated
at these fixed-point temperatures is calibrated by interpolation up to the high temperature
of 3445°C, the calibration accuracy thereof is markedly improved. And, even if the
thermometer is calibrated by extrapolation using any of the fixed-point temperatures,
extrapolation accuracy can be greatly improved as compared with a conventional method,
since the calibration is carried out at a temperature that is higher than the copper
point.
[0032] Figure 6 shows a first embodiment of the fixed-point temperature realizing apparatus
according to the present invention. As a specific example of the fixed-point cell,
a fixed-point cell 4 is used comprising the crucible 1 in which is cast the titanium
carbide-carbon eutectic structure 2 composed of titanium to which 30 wt% of carbon
is added. The cell is placed in a transverse temperature-variable electric furnace.
The temperature-variable furnace includes a carbon furnace core tube 5 that is heated
by direct current flow, and a heat insulator 7 that covers the core tube 5. The interior
of the furnace is evacuated to a vacuum and the interior is then charged with an inert
gas atmosphere. A carbon heat insulator 8 is inserted around the fixed-point cell
4 to increase the uniformity of the temperature distribution and to improve the electrical
insulation between the furnace core tube 5 and the fixed-point cell 4. The blackbody
cavity 3 is formed at one end of the fixed-point cell. A radiation thermometer 9 to
be calibrated, provided outside the furnace, measures the temperature of the fixed-point
cell by detecting the light radiated from the blackbody cavity 3 through a quartz
glass sight hole 10. The internal temperature of the furnace is monitored from the
other end of the furnace by another radiation thermometer 6, providing an output signal
that is input to a control unit (not shown) that controls the heating current.
[0033] Figure 7 shows an example of the output of a radiation thermometer to be calibrated
used to measure the cell Lemperature. This shows that melting and freezing plateaus
can be observed, showing that calibration at the fixed-point temperature is possible.
[0034] Figure 8 shows a second embodiment of the fixed-point temperature realizing apparatus
of the invention. With reference to Figure 8, a fixed-point cell 14 containing a carbide-carbon
eutectic structure is disposed in a vertical temperature-variable electric furnace.
The temperature-variable furnace includes a carbon furnace core tube 11, heater elements
12 around the furnace core tube 11, and heat insulators 13 around the heater elements
12. The core tube 11 interior is evacuated and then charged with an inert gas.
[0035] A blackbody cavity 15 is formed in the upper part of the fixed-point cell 14. A radiation
thermometer 16 to be calibrated, provided outside the furnace, measures the temperature
of the fixed-point cell 14 by detecting the light radiated from the blackbody cavity
15 through a purge unit 17 with no sight hole. A thermocouple 18 inserted into the
furnace from the lower end thereof is used to monitor the internal temperature of
the furnace. To increase the uniformity of the temperature distribution around the
fixed-point cell 14, control radiation thermometers 19 are used to control the heater
elements 12 by dividing the heating control into an upper zone, a middle zone and
a lower zone. With the apparatus thus configured, to calibrate the radiation thermometer
16, the thermometer 16 is used to measure temperature variation of the fixed-point
cell 14 when the temperature around the fixed-point cell 14 is increased and decreased.
The correlation between the thermometer output and the fixed-point temperature values
is used to provide the calibration.
[0036] While the present invention has been described with reference to the above embodiments,
the invention is not limited to the embodiments but may be embodied in various ways
within the scope of the invention as defined in the appended claims. While, for example,
the thermometers to be calibrated have been described with reference to radiation
thermometers, the invention is not limited thereto, it being possible to calibrate
other types of thermometers such as a thermocouple, a fiber-optic thermometer, and
so forth.
[0037] In contrast to the prior art in which adequate accuracy could not be attained owing
to the fact that at temperatures above the copper point of 1085°C, it was necessary
to rely on extrapolation, with the present invention high-temperature calibration
of radiation thermometers, thermocouples and other thermometers can be effected using
interpolation, so accuracy is markedly improved. In the prior art calibration particularly
using a metal-carbon eutectic as the fixed-point material, the fixed-point temperature
that can be realized is up to 2474°C. At temperatures higher than 2474°C the temperature
scale have to be defined by extrapolation. This results in an increase in accuracy
deterioration as the temperature higher than 2474°C increases. In the present invention
using a carbide-carbon eutectic as the fixed-point material, however, the temperature
up to 3445°C can be realized to reduce the accuracy error to 1/4 at 3000°C and at
4000°C enhance the accuracy by one order of magnitude, as compared with that of the
prior art using a carbon-metal eutectic.
[0038] The present invention also makes it possible to maintain the temperature scale by
utilizing a radiation thermometer calibrated at the fixed point temperature without
using a standard ribbon lamp, as was necessary in the prior art. The present invention
also eliminates the conventional need for evaluating accuracy characteristics of high-precision
standard radiation thermometers, greatly simplifying the calibration operation and
helping to advance the provision of a temperature scale system.
[0039] In addition to the calibration of thermometers, the fixed-point cell can also be
applied in the fields of blackbody radiation measurement and photometrics.
1. A fixed-point cell (4, 14), comprising: a crucible (1) composed of carbon and a fixed-point
material (2) enclosed in the crucible, wherein the fixed-point material is a eutectic
structure of carbide and carbon.
2. A fixed-point temperature realizing apparatus, comprising: a fixed-point cell (4,
14) comprising a crucible (1) composed of carbon and a fixed-point material (2) enclosed
in the crucible that is a eutectic structure of carbide and carbon, and a furnace
(5, 11) having the cell disposed therein for increasing and decreasing an environmental
temperature of the cell and a thermometer (9, 16) to measure temperature variation
in the cell.
3. A calibration method for calibrating a thermometer, the method comprising: enclosing
a fixed-point material (2) that is a eutectic structure of carbide and carbon in a
crucible (1) composed of carbon to form a fixed-point cell (4, 14), raising and lowering
an environmental temperature of the cell, measuring temperature variation of the cell
with a thermometer (9, 16), and calibrating the thermometer based on measured temperature
variation.
4. A fixed-point cell according to claim 1, wherein the carbide is a carbide of any of
boron, molybdenum, vanadium, titanium, zirconium, hafnium, niobium, tantalum, tungsten,
and rare earth elements.
5. A fixed-point temperature realizing apparatus according to claim 2, wherein the carbide
is a carbide of any of boron, molybdenum, vanadium, titanium, zirconium, hafnium,
niobium, tantalum, tungsten, and rare earth elements.
6. A calibration method according to claim 3, wherein the carbide is a carbide of any
of boron, molybdenum, vanadium, titanium, zirconium, hafnium, niobium, tantalum, tungsten,
and rare earth elements.
7. A fixed-point temperature realizing apparatus according to claim 2, wherein the thermometer
is a radiation thermometer.
8. A calibration method according to claim 3, wherein the thermometer is a radiation
thermometer.